mandrin, in your last two models the focus seems to be on the latteral motion of the hips and not so much on the rotational? In the 7th edition homer wanted the stoke pattern to be more of a shift from the top, or slide, and not so much rotational. yes it has to rotate back to square or very close to it but that is a lot less rotation then a tiger woods. what does your science say about homers slide rather then just trying to rotate your hips as far and as fast as you can? we know in kinetic energy that if the hips and shoulders are still rotating there has not been a full transfer of energy. so optimumly kinetic energy wise, they would be square at impact and allow the pendulum to not be comprimised. therefore maximizing the swing
shootin4par,
Rotation is represented by an angular velocity vector. Its magnitude represents the amplitude of the angular velocity and its direction in space is perpendicular to the plane in which the rotation takes place. More accurately in or parallel to this plane. This is illustrated in Fig1.
Fortunately, angular velocities can be added as vectors. This is not the case for angular accelerations. This means, for instance, that we can decompose a rotation into two or more independent rotations, or vice versa, can add them together.
A golfer mainly has two major axes of rotation, one through his spine or perhaps more vertical if he is a tripod-believer.
The other one, a horizontal axis, to account for the rotation in the vertical plane. The latter being caused by the lateral weight shift.
Hence these two rotations can be represented by angular velocity vectors and, as mentioned above, can then be added to find the resulting angular vector and the associated swing plane. This is illustrated in Fig2.
The two rotational motions executed by a golfer hence define a composite plane. Coming back to your question. The lateral (rotational) slide you are referring to in your post can generate substantial kinetic energy, not to be ignored. Moreover as shown in Fig 2 it directly affects the steepness of the composite swing plane.
Thinking of the down swing as a composite action of rotation about two axes is quite instructive. You can think of simultaneous action; different weighting of each rotation; someone with little ‘lateral’ slide needs to ‘drop’ the arms to compensate; also view the downswing plane shift as being due to ending lateral rotational motion, see Fig3.
So far we have considered only two rotational motions of the body. There are also the arms and wrists which have to be considered to complete the picture. However one can have a downswing with very little independent arm motion (ala Dante).